It is worth noting that,
the building blocks in [1]}
have one oscillation direction \(k\) ,
orthogonal to the direction vectors \(k_1\)  and \(k_2\) ,
and have the \(1D\) -intermittency.
In order to control the strong viscosity and resistivity \((-\Delta )^{{\alpha }_i}\) 
when \({\alpha }_i\ge 1/2\) , \(i=1,2\) ,
the idea here to explore more intermittency,
inspired by the work [2]} in the NSE context,
is to introduce the new concentration function \(\psi _{(k_1)}\)  in (REF ).
Two new parameters \(r_{\perp }\)  (the rescaling parameter in the direction vertical to the flow)
and \(r_{\parallel }\)  (the rescaling parameter in the direction parallel to the flow)
parameterize the concentration of the intermittent flows \(W_{(k)}\)  and \(D_{(k)}\) .
In particular,
one has
\(\sum \limits _{k\in \Lambda _u\cup \Lambda _B} \Vert W_{(k)}\Vert _{C_tL^1_x}+ \sum \limits _{k\in \Lambda _B} \Vert D_{(k)}\Vert _{C_tL^1_x}\lesssim r_{\perp }^\frac{1}{2} r_{\parallel }^{\frac{1}{2}} = \lambda _{q+1}^{-1 + 4{\varepsilon }},\) 
